Commutativity of induction and inflation of representations












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Let $G$ be a finite group, $H$ a subgroup and $N$ a normal subgroup. Let $chi$ be a representation of $HN/N$. Does $$Ind_{HN}^G Inf_{HN/N}^{HN} chi = Inf_{G/N}^G Ind_{HN/N}^{G/N} chi$$ always hold? Here $Ind$ and $Inf$ are the induction and inflation functors.



If this isn't true, are there any simple sufficient conditions for it to hold (possibly with a sketch proof/reference)?










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    2












    $begingroup$


    Let $G$ be a finite group, $H$ a subgroup and $N$ a normal subgroup. Let $chi$ be a representation of $HN/N$. Does $$Ind_{HN}^G Inf_{HN/N}^{HN} chi = Inf_{G/N}^G Ind_{HN/N}^{G/N} chi$$ always hold? Here $Ind$ and $Inf$ are the induction and inflation functors.



    If this isn't true, are there any simple sufficient conditions for it to hold (possibly with a sketch proof/reference)?










    share|cite|improve this question









    $endgroup$















      2












      2








      2


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      $begingroup$


      Let $G$ be a finite group, $H$ a subgroup and $N$ a normal subgroup. Let $chi$ be a representation of $HN/N$. Does $$Ind_{HN}^G Inf_{HN/N}^{HN} chi = Inf_{G/N}^G Ind_{HN/N}^{G/N} chi$$ always hold? Here $Ind$ and $Inf$ are the induction and inflation functors.



      If this isn't true, are there any simple sufficient conditions for it to hold (possibly with a sketch proof/reference)?










      share|cite|improve this question









      $endgroup$




      Let $G$ be a finite group, $H$ a subgroup and $N$ a normal subgroup. Let $chi$ be a representation of $HN/N$. Does $$Ind_{HN}^G Inf_{HN/N}^{HN} chi = Inf_{G/N}^G Ind_{HN/N}^{G/N} chi$$ always hold? Here $Ind$ and $Inf$ are the induction and inflation functors.



      If this isn't true, are there any simple sufficient conditions for it to hold (possibly with a sketch proof/reference)?







      reference-request finite-groups representation-theory






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      asked Feb 9 '17 at 14:33









      Matt BMatt B

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          $begingroup$

          Let $tau$ be an irreducible subrepresentation of $Ind_{HN}^GInf_{HN/N}^{HN}chi$, so by Frobenius reciprocity there's a non-zero map $tau|_{HN}rightarrow Inf_{HN/N}^{HN}chi$. So $N$ acts trivially through $tau$, meaning that we can identify $tau|_{HN}$ with a representation of $HN/N$, and doing so we get a non-zero map $tau|_{HN}rightarrowchi$. Using Frobenius reciprocity again, $tau$ is a subrepresentation of $Ind_{HN/N}^{G/N}chi$, and inflating gives a non-zero map $taurightarrow Inf_{G/N}^GInd_{HN/N}^{G/N}chi$. So every irreducible subrepresentation of the left hand side is a subrepresentation of the right hand side. That means that the only way that the two representations can't be equal is if some subrepresentations appear with different multiplicities, but since $|G/HN|=|G|/|HN|=|G||Hcap N|/|HN|=|G/N|/|H/Hcap N|=|G/N|/|HN/N|$, you can compare dimensions to conclude that the representations genuinely are equal.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
            $endgroup$
            – Matt B
            Feb 10 '17 at 14:35



















          0












          $begingroup$

          Yes, it holds (as long as your equality sign stands for canonical isomorphism). See Exercise 4.1.11 in Darij Grinberg and Victor Reiner, Hopf algebras and combinatorics, 11 May 2018, arXiv:1409.8356v5 (see the ancillary file for the solution). Note that our $K$, $H$ and $G$ correspond to your $N$, $HN$ and $G$.






          share|cite|improve this answer











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            2 Answers
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            2 Answers
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            active

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            $begingroup$

            Let $tau$ be an irreducible subrepresentation of $Ind_{HN}^GInf_{HN/N}^{HN}chi$, so by Frobenius reciprocity there's a non-zero map $tau|_{HN}rightarrow Inf_{HN/N}^{HN}chi$. So $N$ acts trivially through $tau$, meaning that we can identify $tau|_{HN}$ with a representation of $HN/N$, and doing so we get a non-zero map $tau|_{HN}rightarrowchi$. Using Frobenius reciprocity again, $tau$ is a subrepresentation of $Ind_{HN/N}^{G/N}chi$, and inflating gives a non-zero map $taurightarrow Inf_{G/N}^GInd_{HN/N}^{G/N}chi$. So every irreducible subrepresentation of the left hand side is a subrepresentation of the right hand side. That means that the only way that the two representations can't be equal is if some subrepresentations appear with different multiplicities, but since $|G/HN|=|G|/|HN|=|G||Hcap N|/|HN|=|G/N|/|H/Hcap N|=|G/N|/|HN/N|$, you can compare dimensions to conclude that the representations genuinely are equal.






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
              $endgroup$
              – Matt B
              Feb 10 '17 at 14:35
















            2












            $begingroup$

            Let $tau$ be an irreducible subrepresentation of $Ind_{HN}^GInf_{HN/N}^{HN}chi$, so by Frobenius reciprocity there's a non-zero map $tau|_{HN}rightarrow Inf_{HN/N}^{HN}chi$. So $N$ acts trivially through $tau$, meaning that we can identify $tau|_{HN}$ with a representation of $HN/N$, and doing so we get a non-zero map $tau|_{HN}rightarrowchi$. Using Frobenius reciprocity again, $tau$ is a subrepresentation of $Ind_{HN/N}^{G/N}chi$, and inflating gives a non-zero map $taurightarrow Inf_{G/N}^GInd_{HN/N}^{G/N}chi$. So every irreducible subrepresentation of the left hand side is a subrepresentation of the right hand side. That means that the only way that the two representations can't be equal is if some subrepresentations appear with different multiplicities, but since $|G/HN|=|G|/|HN|=|G||Hcap N|/|HN|=|G/N|/|H/Hcap N|=|G/N|/|HN/N|$, you can compare dimensions to conclude that the representations genuinely are equal.






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
              $endgroup$
              – Matt B
              Feb 10 '17 at 14:35














            2












            2








            2





            $begingroup$

            Let $tau$ be an irreducible subrepresentation of $Ind_{HN}^GInf_{HN/N}^{HN}chi$, so by Frobenius reciprocity there's a non-zero map $tau|_{HN}rightarrow Inf_{HN/N}^{HN}chi$. So $N$ acts trivially through $tau$, meaning that we can identify $tau|_{HN}$ with a representation of $HN/N$, and doing so we get a non-zero map $tau|_{HN}rightarrowchi$. Using Frobenius reciprocity again, $tau$ is a subrepresentation of $Ind_{HN/N}^{G/N}chi$, and inflating gives a non-zero map $taurightarrow Inf_{G/N}^GInd_{HN/N}^{G/N}chi$. So every irreducible subrepresentation of the left hand side is a subrepresentation of the right hand side. That means that the only way that the two representations can't be equal is if some subrepresentations appear with different multiplicities, but since $|G/HN|=|G|/|HN|=|G||Hcap N|/|HN|=|G/N|/|H/Hcap N|=|G/N|/|HN/N|$, you can compare dimensions to conclude that the representations genuinely are equal.






            share|cite|improve this answer









            $endgroup$



            Let $tau$ be an irreducible subrepresentation of $Ind_{HN}^GInf_{HN/N}^{HN}chi$, so by Frobenius reciprocity there's a non-zero map $tau|_{HN}rightarrow Inf_{HN/N}^{HN}chi$. So $N$ acts trivially through $tau$, meaning that we can identify $tau|_{HN}$ with a representation of $HN/N$, and doing so we get a non-zero map $tau|_{HN}rightarrowchi$. Using Frobenius reciprocity again, $tau$ is a subrepresentation of $Ind_{HN/N}^{G/N}chi$, and inflating gives a non-zero map $taurightarrow Inf_{G/N}^GInd_{HN/N}^{G/N}chi$. So every irreducible subrepresentation of the left hand side is a subrepresentation of the right hand side. That means that the only way that the two representations can't be equal is if some subrepresentations appear with different multiplicities, but since $|G/HN|=|G|/|HN|=|G||Hcap N|/|HN|=|G/N|/|H/Hcap N|=|G/N|/|HN/N|$, you can compare dimensions to conclude that the representations genuinely are equal.







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Feb 9 '17 at 18:23









            PL.PL.

            1,58188




            1,58188












            • $begingroup$
              Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
              $endgroup$
              – Matt B
              Feb 10 '17 at 14:35


















            • $begingroup$
              Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
              $endgroup$
              – Matt B
              Feb 10 '17 at 14:35
















            $begingroup$
            Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
            $endgroup$
            – Matt B
            Feb 10 '17 at 14:35




            $begingroup$
            Can you elaborate on what happens with the multiplicities? If $dim tau_1 =dim tau_2$ then the dimension argument doesn't work if say $Ind Inf chi = tau_1 oplus 2 tau_2$ as it allows for $Inf Ind chi = 2tau_1 oplus tau_2$.
            $endgroup$
            – Matt B
            Feb 10 '17 at 14:35











            0












            $begingroup$

            Yes, it holds (as long as your equality sign stands for canonical isomorphism). See Exercise 4.1.11 in Darij Grinberg and Victor Reiner, Hopf algebras and combinatorics, 11 May 2018, arXiv:1409.8356v5 (see the ancillary file for the solution). Note that our $K$, $H$ and $G$ correspond to your $N$, $HN$ and $G$.






            share|cite|improve this answer











            $endgroup$


















              0












              $begingroup$

              Yes, it holds (as long as your equality sign stands for canonical isomorphism). See Exercise 4.1.11 in Darij Grinberg and Victor Reiner, Hopf algebras and combinatorics, 11 May 2018, arXiv:1409.8356v5 (see the ancillary file for the solution). Note that our $K$, $H$ and $G$ correspond to your $N$, $HN$ and $G$.






              share|cite|improve this answer











              $endgroup$
















                0












                0








                0





                $begingroup$

                Yes, it holds (as long as your equality sign stands for canonical isomorphism). See Exercise 4.1.11 in Darij Grinberg and Victor Reiner, Hopf algebras and combinatorics, 11 May 2018, arXiv:1409.8356v5 (see the ancillary file for the solution). Note that our $K$, $H$ and $G$ correspond to your $N$, $HN$ and $G$.






                share|cite|improve this answer











                $endgroup$



                Yes, it holds (as long as your equality sign stands for canonical isomorphism). See Exercise 4.1.11 in Darij Grinberg and Victor Reiner, Hopf algebras and combinatorics, 11 May 2018, arXiv:1409.8356v5 (see the ancillary file for the solution). Note that our $K$, $H$ and $G$ correspond to your $N$, $HN$ and $G$.







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Jan 6 at 15:33

























                answered Feb 9 '17 at 18:58









                darij grinbergdarij grinberg

                11.5k33168




                11.5k33168






























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